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Airborne Gravity 2010 - Geoscience Australia

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<strong>Airborne</strong> <strong>Gravity</strong> <strong>2010</strong><br />

Performance of the Gedex High-Definition <strong>Airborne</strong><br />

<strong>Gravity</strong> Gradiometer<br />

Summary<br />

Kieran A. Carroll 1 , David Hatch 2 , and Brian Main 3<br />

1 Gedex Inc., Toronto Canada (Kieran.Carroll@Gedex.ca)<br />

2 Gedex Inc., Toronto Canada (David.Hatch@Gedex.ca)<br />

3 Gedex Inc., Toronto Canada (Brian.Main@Gedex.ca)<br />

In this paper, we provide a high-level description of the design for the Gedex High Definition <strong>Airborne</strong><br />

<strong>Gravity</strong> Gradiometer (HD-AGG) system, and show the performance achieved by several of the<br />

elements of the system.<br />

Introduction<br />

The goal for Gedex is to develop a commercially viable airborne gravity gradiometer that achieves<br />

post-process performance of 1 E/Hz 1/2 from 0.001 to 1 Hz. At a typical flying height and survey speed<br />

this will produce gravity gradient survey data with a spatial resolution of 50-100 m and an RMS noise<br />

of 1 E. To be productive in a survey aircraft, the system must produce data within this noise<br />

specification while flying at a standard survey height of 80 m in turbulence conditions up to 1 m/s 2 .<br />

The technical hurdles that must be overcome to achieve the noise specifications are formidable. The<br />

instrument must be able to measure displacements of the proof masses to accuracy on the order of<br />

10 -13 m which is about 1000 times smaller than the diameter of a hydrogen atom. As well, no gravity<br />

gradiometer can distinguish between gravity gradient and angular velocity, requiring that the<br />

instrument must be rotationally stabilized to within 0.06 deg/s. To achieve these and other extreme<br />

specifications, Gedex is developing a highly sophisticated system comprised of a number of key subsystems.<br />

The major components that make up the Gedex High-definition <strong>Airborne</strong> <strong>Gravity</strong><br />

Gradiometer system are as follows: gravity gradiometer instrument, cryostat, isolation mount, control<br />

system, aircraft and post-processing software. Figure 1 shows the flight components of the system,<br />

mounted in a Cessna 208. At the time of writing this paper (mid-<strong>2010</strong>), all subsystems have been built,<br />

assemblies of some of these subsystems have been flight-tested, and preparations are underway for<br />

flight-testing the complete, integrated system.<br />

The gravity gradiometer instrument being developed for the HD-AGG is of the Cross-Component<br />

Gradiometer type. This class of instrument has been independently demonstrated (Anstie et al., 2009)<br />

to have acquired signal at sub-eotvos levels in a laboratory setting. The challenge faced by Gedex is<br />

achieving the same level of performance on a moving platform. As it is impossible to build a<br />

gradiometer that is totally insensitive to common mode accelerations, it is important to be able to<br />

minimize the effects of these. One can remove the linear motion-induced noise that can be estimated<br />

with independent accelerometers. As this compensation process cannot totally remove motion induced<br />

noise, Gedex is also developing a motion isolation system to attenuate the aircraft accelerations that<br />

the instrument experiences. The isolation mount will also protect the instrument from large<br />

accelerations.<br />

The end-to-end performance achieved by this system, in terms of the noise level of the gravity<br />

gradiometry data reported after post-processing, is dependent on its various subsystems meeting their<br />

own performance targets. Here we show the level of performance achieved by several of the HD-AGG<br />

subsystems, in particular the gravity gradiometer instrument, the cryostat, the motion isolation mount,<br />

and the post-processing software.<br />

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